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In the title compound, (C
10H
10N
2)[PdCl
4], the Pd atom in the tetrachloridopalladate anion exhibits a square-planar geometry. The anion is hydrogen bonded to the bipyridinium cation by an N—H
Cl hydrogen bond to form chains. The bipyridinium cation and the tetrachloridopalladate anion exhibit perfect 2/
m symmetry with the Pd atom located on a 2/
m symmetry site.
Supporting information
CCDC reference: 640319
Key indicators
- Single-crystal X-ray study
- T = 298 K
- Mean (C-C) = 0.005 Å
- R factor = 0.023
- wR factor = 0.058
- Data-to-parameter ratio = 13.3
checkCIF/PLATON results
No syntax errors found
Alert level C
PLAT128_ALERT_4_C Non-standard setting of Space group C2/m .... I2/m
0 ALERT level A = In general: serious problem
0 ALERT level B = Potentially serious problem
1 ALERT level C = Check and explain
0 ALERT level G = General alerts; check
0 ALERT type 1 CIF construction/syntax error, inconsistent or missing data
0 ALERT type 2 Indicator that the structure model may be wrong or deficient
0 ALERT type 3 Indicator that the structure quality may be low
1 ALERT type 4 Improvement, methodology, query or suggestion
0 ALERT type 5 Informative message, check
Data collection: SMART (Bruker, 2006); cell refinement: SMART; data reduction: SAINT (Bruker, 2006); program(s) used to solve structure: SHELXTL (Sheldrick, 2000); program(s) used to refine structure: SHELXTL; molecular graphics: X-SEED (Barbour, 2001); software used to prepare material for publication: publCIF Westrip, 2007) and enCIFer (Allen et al., 2004).
4,4'-Bipyridinium tetrachloridopalladate(II)
top
Crystal data top
(C10H10N2)[PdCl4] | F(000) = 396 |
Mr = 406.40 | Dx = 2.133 Mg m−3 |
Monoclinic, I2/m | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -I 2y | Cell parameters from 2186 reflections |
a = 6.718 (1) Å | θ = 3.1–25.4° |
b = 11.754 (2) Å | µ = 2.29 mm−1 |
c = 8.015 (2) Å | T = 298 K |
β = 90.649 (3)° | Prism, yellow |
V = 632.9 (2) Å3 | 0.19 × 0.08 × 0.07 mm |
Z = 2 | |
Data collection top
Bruker SMART APEX CCD diffractometer | 613 independent reflections |
Radiation source: fine-focus sealed tube | 591 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.037 |
Detector resolution: 0.661 pixels mm-1 | θmax = 25.4°, θmin = 3.1° |
ω scans | h = −8→8 |
Absorption correction: analytical (Sheldrick, 2000) | k = −14→14 |
Tmin = 0.670, Tmax = 0.855 | l = −9→9 |
2552 measured reflections | |
Refinement top
Refinement on F2 | Primary atom site location: structure-invariant direct methods |
Least-squares matrix: full | Secondary atom site location: difference Fourier map |
R[F2 > 2σ(F2)] = 0.023 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.058 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.10 | w = 1/[σ2(Fo2) + (0.0295P)2 + 0.5871P] where P = (Fo2 + 2Fc2)/3 |
613 reflections | (Δ/σ)max < 0.001 |
46 parameters | Δρmax = 0.58 e Å−3 |
1 restraint | Δρmin = −0.29 e Å−3 |
Special details top
Experimental. The non-standard setting I2/m for the space group C2/m was selected following
the suggestions of Alan D. Mighell (Mighell, 2002) for monoclinic conventional
cells |
Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes)
are estimated using the full covariance matrix. The cell e.s.d.'s are taken
into account individually in the estimation of e.s.d.'s in distances, angles
and torsion angles; correlations between e.s.d.'s in cell parameters are only
used when they are defined by crystal symmetry. An approximate (isotropic)
treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s.
planes. |
Refinement. Refinement of F2 against ALL reflections. The weighted R-factor
wR and goodness of fit S are based on F2, conventional
R-factors R are based on F, with F set to zero for
negative F2. The threshold expression of F2 >
σ(F2) is used only for calculating R-factors(gt) etc.
and is not relevant to the choice of reflections for refinement.
R-factors based on F2 are statistically about twice as large
as those based on F, and R- factors based on ALL data will be
even larger. |
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top | x | y | z | Uiso*/Ueq | |
Pd1 | 1.0000 | 0.0000 | 0.0000 | 0.03097 (18) | |
Cl1 | 0.79728 (13) | 0.13796 (7) | 0.10751 (11) | 0.0519 (3) | |
N1 | 0.4434 (6) | 0.0000 | 0.2829 (5) | 0.0489 (10) | |
H1 | 0.558 (4) | 0.0000 | 0.234 (6) | 0.059* | |
C2 | 0.3630 (5) | 0.0972 (3) | 0.3246 (5) | 0.0560 (9) | |
H2 | 0.4243 | 0.1651 | 0.2950 | 0.067* | |
C3 | 0.1888 (5) | 0.0993 (3) | 0.4116 (5) | 0.0502 (8) | |
H3 | 0.1330 | 0.1686 | 0.4417 | 0.060* | |
C4 | 0.0965 (6) | 0.0000 | 0.4544 (5) | 0.0333 (9) | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
Pd1 | 0.0321 (3) | 0.0306 (3) | 0.0304 (3) | 0.000 | 0.00733 (17) | 0.000 |
Cl1 | 0.0506 (6) | 0.0374 (5) | 0.0684 (6) | 0.0049 (3) | 0.0275 (4) | −0.0009 (4) |
N1 | 0.035 (2) | 0.074 (3) | 0.038 (2) | 0.000 | 0.0092 (16) | 0.000 |
C2 | 0.048 (2) | 0.056 (2) | 0.065 (2) | −0.0062 (18) | 0.0137 (17) | 0.0120 (18) |
C3 | 0.0444 (19) | 0.0395 (19) | 0.067 (2) | −0.0008 (14) | 0.0182 (16) | 0.0016 (16) |
C4 | 0.034 (2) | 0.036 (2) | 0.0301 (19) | 0.000 | 0.0019 (16) | 0.000 |
Geometric parameters (Å, º) top
Pd1—Cl1 | 2.2920 (8) | C2—H2 | 0.9300 |
N1—C2i | 1.309 (4) | C3—C4 | 1.367 (4) |
N1—C2 | 1.309 (4) | C3—H3 | 0.9300 |
N1—H1 | 0.87 (3) | C4—C3i | 1.367 (4) |
C2—C3 | 1.369 (5) | C4—C4ii | 1.496 (8) |
| | | |
Cl1iii—Pd1—Cl1 | 89.94 (4) | C3—C2—H2 | 119.9 |
Cl1i—Pd1—Cl1 | 90.06 (4) | C4—C3—C2 | 120.3 (3) |
Cl1iv—Pd1—Cl1 | 180.00 (5) | C4—C3—H3 | 119.8 |
C2i—N1—C2 | 121.6 (4) | C2—C3—H3 | 119.8 |
C2i—N1—H1 | 119.1 (3) | C3i—C4—C3 | 117.2 (4) |
C2—N1—H1 | 119.1 (3) | C3i—C4—C4ii | 121.4 (2) |
N1—C2—C3 | 120.2 (4) | C3—C4—C4ii | 121.4 (2) |
N1—C2—H2 | 119.9 | | |
Symmetry codes: (i) x, −y, z; (ii) −x, −y, −z+1; (iii) −x+2, y, −z; (iv) −x+2, −y, −z. |
Hydrogen-bond geometry (Å, º) top
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1···Cl1 | 0.87 (3) | 2.51 (3) | 3.214 (3) | 139 (1) |
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